# Ethylene frontier orbitals with PBE and B3LYP Ethylene was built from the SMILES string `C=C` and optimized once with ADF at PBE/DZP. Two single-point calculations, PBE/DZP and B3LYP/DZP, then used that same geometry. Both calculations used an all-electron DZP basis and Normal numerical quality. Orbital energies are Kohn-Sham eigenvalues in eV. ## Optimized geometry The optimized C=C distance is 1.3320 Å. ![Optimized ethylene geometry](figures/optimized_ethylene.png) ## Frontier orbital energies | Method | HOMO (eV) | LUMO (eV) | Gap (eV) | |:----------|------------:|------------:|-----------:| | PBE/DZP | -7.0061 | -1.1879 | 5.8182 | | B3LYP/DZP | -7.7749 | -0.2106 | 7.5642 | The nearest three occupied and three virtual orbitals are: | Method | Orbital | Energy (eV) | Occupation | |:----------|:----------|--------------:|-------------:| | PBE/DZP | HOMO-2 | -10.4784 | 2.0 | | PBE/DZP | HOMO-1 | -8.7810 | 2.0 | | PBE/DZP | HOMO | -7.0061 | 2.0 | | PBE/DZP | LUMO | -1.1879 | 0.0 | | PBE/DZP | LUMO+1 | 0.8367 | 0.0 | | PBE/DZP | LUMO+2 | 1.9669 | 0.0 | | B3LYP/DZP | HOMO-2 | -11.7766 | 2.0 | | B3LYP/DZP | HOMO-1 | -9.9698 | 2.0 | | B3LYP/DZP | HOMO | -7.7749 | 2.0 | | B3LYP/DZP | LUMO | -0.2106 | 0.0 | | B3LYP/DZP | LUMO+1 | 1.3945 | 0.0 | | B3LYP/DZP | LUMO+2 | 2.5806 | 0.0 | ![Frontier orbital energy-level diagram](figures/frontier_energy_levels.png) ## HOMO and LUMO isosurfaces The four orbital pictures below were generated by `amsreport` from the corresponding ADF engine result files. Contrasting colors mark opposite orbital phases. | Method | HOMO | LUMO | |---|---|---| | PBE/DZP | ![PBE HOMO](figures/amsreport_pbe_homo/report.jpgs/0.jpg) | ![PBE LUMO](figures/amsreport_pbe_lumo/report.jpgs/0.jpg) | | B3LYP/DZP | ![B3LYP HOMO](figures/amsreport_b3lyp_homo/report.jpgs/0.jpg) | ![B3LYP LUMO](figures/amsreport_b3lyp_lumo/report.jpgs/0.jpg) | ## Conclusion At this fixed PBE geometry, replacing PBE with B3LYP changes the Kohn-Sham HOMO-LUMO gap by +1.7460 eV. The HOMO and LUMO isosurfaces allow the comparison to distinguish an energy shift from a qualitative change in orbital shape. These Kohn-Sham gaps are method-dependent orbital-energy differences, not optical excitation energies. ## Calculation inputs ### PBE/DZP geometry optimization ```ams Task GeometryOptimization System Atoms C 0.6644850805 0.0279879686 -0.0236852009 C -0.6644849893 -0.0279879318 0.0236851499 H 1.2534332310 -0.8786144292 0.0702991539 H 1.1670384263 0.9805640030 -0.1565753856 H -1.2534332920 0.8786143859 -0.0702991171 H -1.1670384566 -0.9805639965 0.1565753997 End BondOrders 1 2 2.0 1 3 1.0 1 4 1.0 2 5 1.0 2 6 1.0 End End Engine adf Basis Core None Type DZP End NumericalQuality Normal SCF Iterations 100 End XC GGA PBE End EndEngine ``` ### PBE/DZP single point ```ams Task SinglePoint System Atoms C 0.6649813115 0.0278988522 -0.0242986367 C -0.6649810155 -0.0278982997 0.0243008447 H 1.2789279657 -0.8699226278 0.0686049752 H 1.1932069166 0.9740820859 -0.1564006741 H -1.2789292580 0.8699198605 -0.0686220517 H -1.1932059203 -0.9740798711 0.1564155425 End BondOrders 1 2 2.0 1 3 1.0 1 4 1.0 2 5 1.0 2 6 1.0 End End Engine adf Basis Core None Type DZP End NumericalQuality Normal SCF Iterations 100 End XC GGA PBE End EndEngine ``` ### B3LYP/DZP single point ```ams Task SinglePoint System Atoms C 0.6649813115 0.0278988522 -0.0242986367 C -0.6649810155 -0.0278982997 0.0243008447 H 1.2789279657 -0.8699226278 0.0686049752 H 1.1932069166 0.9740820859 -0.1564006741 H -1.2789292580 0.8699198605 -0.0686220517 H -1.1932059203 -0.9740798711 0.1564155425 End BondOrders 1 2 2.0 1 3 1.0 1 4 1.0 2 5 1.0 2 6 1.0 End End Engine adf Basis Core None Type DZP End NumericalQuality Normal SCF Iterations 100 End XC Hybrid B3LYP End EndEngine ```